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机译:0.5BaTiO_3-0.5Bi(Mg_(1/2)Ti_(1/2))O_3电陶瓷中的类偶极玻璃弛豫铁电行为
Research School of Chemistry, The Australian National University, Canberra, ACT 0200, Australia;
Research School of Chemistry, The Australian National University, Canberra, ACT 0200, Australia;
Research School of Chemistry, The Australian National University, Canberra, ACT 0200, Australia;
Research School of Chemistry, The Australian National University, Canberra, ACT 0200, Australia;
Research School of Chemistry, The Australian National University, Canberra, ACT 0200, Australia;
Electronic Materials Research Laboratory (EMRL), Xian Jiaotong University, Shaanxi 710049, China;
Electronic Materials Research Laboratory (EMRL), Xian Jiaotong University, Shaanxi 710049, China;
机译:铁电弛豫行为Ba_(1-x)A_x(Ti_(0.7)Zr_(0.3))O_3和Ba_(1-x)A'_(2x / 3)square_(x / 3)(Ti_(0.7)Zr_( 0.3))O_3成分(A = Ca,Sr; A'= Y,La,Bi)
机译:(1-x)(Bi_(0.5)Na_(0.5))_(0.06)Ba_(0.06)TiO_3-XBI(Mg_(0.5)Ti_(0.5)O_3松弛剂铁电薄膜
机译:电场下0.85 Ba(Ti0.96Zr0.04)O_3-0.15 Bi(Mg_(0.5)Ti_(0.5))O_3弛豫铁电的介电响应:PNR的演化
机译:BaTiO_3-Bi(Mg_(1/2)Ti_(1/2))O_3陶瓷的弛豫特性
机译:核壳结构和弛豫铁电材料在电能存储方面的进展
机译:超薄弛豫铁电薄膜中的铁电和自极化
机译:弛豫场冷却效应的中子衍射研究 铁电体pb [(Zn_ {1/3} Nb_ {2/3})_ {0.92} Ti_ {0.08}] O_ {3}